Jennifer R. Luker
Vice President
The MuShield Co. Inc.
Goffstown, N.H.

Magnetic shielding protects electronic circuits from magnetic-field interference. Usually, sources of this interference include permanent magnets, transformers, motors, solenoids, and cables. Magnetic shields provide a path around sensitive areas to deflect magnetic flux. In addition, shielding may contain magnetic flux around a component that generates flux.

The ability to conduct magnetic lines of force is called permeability, and in a magnetic shield, the degree of permeability is expressed numerically. The standard or base line is free space with a rating of one, compared to shield materials which range from about 200 to 350,000.

Shields handle two basic needs. One prevents strong field radiation from sources such as transformers, magnets, and motors. The second shields instruments and devices from magnetic fields in an environment or prevents emanation from other sources. Three general types of materials are used for these — high permeability, medium permeability, and high saturation.

High-permeability materials have a minimum value of 80,000 at B-40 and a maximum of 350,000 with a saturation point of about 7,500 gauss after heat treating. Medium-permeability materials are usually used with high-permeability materials and have values of 12,500 to 150,000 with a saturation point of about 15,500 gauss. Highsaturation materials have permeability ranging from 200 to 50,000 with saturation points between 18,000 and 21,000 gauss.

Magnetic fields: To determine the approximate magnetic field in the shield

 

 

For example, a shield 1.5 in. in diameter

made of material 0.06 in. thick in a field of 80 gauss has a flux density of 2,500.

 

 

Shield thickness: For selection of shield thickness for fields of less than 2 gauss,

 

 

A shield 1.5 in. in diameter with a permeability of 80,000 and attenuation field of 1,000 to 1.0 would need a shield 0.019-in. thick.

 

 

Efficient shielding: When considering the price of materials, maintaining the correct thickness keeps costs to a minimum. The magnetic-shielding material must have an initial permeability of at least 80,000, otherwise the shield thickness is compromised.

When a strong field is encountered, a thickness can be selected that develops maximum permeability in the material. For instance, a flux density in the shield of 2,300 to 2,500 gauss produces maximum permeability in the material. To determine the required thickness

 

 

For a sense of scale, a shield 6 in. long and 1.5 in. in diameter in an 80-gauss field requires a shield 0.06 in. thick;

 

 

Field attenuation: To determine the attenuation of a field (ratio),

 

 

Using the above factors, the attenuation field is found to be 14,000 for a shielding material with permeability of 350,000.

 

 

Flux density: To determine the flux density within the shield in gauss

 

 

Here, a flux density of 0.0057 gauss is present within the shield when a field of 80 gauss exists outside the shield and an attenuation of 14,000 has been achieved;

 

 

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